Quasistars and the cosmic evolution of massive black holes

TL;DR

This paper models the formation and evolution of massive black hole seeds within quasistars, linking their properties to galaxy mergers and gravitational instability, and predicts their observability with JWST.

Contribution

It introduces a merger-tree based model connecting quasistar formation to galaxy dynamics and compares seed black hole growth from quasistars with stellar remnants.

Findings

Models reproduce observed high-redshift quasar densities.

Predicted quasistar mass function peaks at ~10^6 solar masses.

JWST could detect several quasistars at redshifts 5-10.

Abstract

We explore the cosmic evolution of massive black hole (MBH) seeds forming within 'quasistars' (QSs), accreting black holes embedded within massive hydrostatic gaseous envelopes. These structures could form if the infall of gas into the center of a halo exceeds about 1 solar mass per year. We use a merger-tree approach to estimate the rate at which QSs might form as a function of redshift, and the statistical properties of the resulting QS and seed black hole populations. We relate the triggering of runaway infall to major mergers of gas-rich galaxies, and to a threshold for global gravitational instability, which we link to the angular momentum of the host. This is the main parameter of our models. Once infall is triggered, its rate is determined by the halo potential; the properties of the resulting QS and seed black hole depend on this rate. After the epoch of QSs, we model the growth of MBHs within their hosts in a merger-driven accretion scenario. We compare MBH seeds grown inside quasistars to a seed model that derives from the remnants of the first metal-free stars, and also study the case in which both channels of MBH formation operate simultaneously. We find that a limited range of QS/MBH formation efficiencies exists that allows one to reproduce observational constraints. Our models match the density of z = 6 quasars, the cumulative mass density accreted onto MBHs (according to Soltan's argument), and the current mass density of MBHs. The mass function of QSs peaks at mass ~ 1e6 solar masses, and we calculate the number counts for the JWST in the 2-10 micron band. We find that JWST could detect up to several QSs per field at z ~ 5 - 10.